Type-II second-harmonic-generation properties of YCOB and GdCOB single crystals.

As excellent nonlinear optical (NLO) crystals, YCa(4)O(BO(3))(3) (YCOB) and GdCa(4)O(BO(3))(3) (GdCOB) have been paid much attention since their first appearance in 1990's. From that time to now, almost all of related researches and applications have focused on their type-I phase-matching (PM) configurations which possess large effective NLO coefficient (d(eff)). In this paper, type-II second-harmonic-generation (SHG) properties of these two crystals are reported, including PM curve, d(eff), angular acceptance and walk-off angle. Both of the type-II SHG experiments for 1064 and 1320 nm have indicated that the optimum directions which have maximum d(eff) locate in the second octant, i.e. (90° < θ< 180°, 0° < ϕ < 90°). For a (112°, 81.3°)-cut, 24 mm long YCOB crystal, the largest type-II SHG conversion efficiency of a 1064 nm Nd:YAG pico-second laser is 55%, which reaches the same level of the optimum type-I sample. To our knowledge this is the first time that type-II SHG performance of YCOB and GdCOB crystals is investigated intensively. Our research has shown that the smaller d(eff) of type-II PM can be compensated by its larger angular acceptance and less beam walk-off. The same level SHG conversion efficiency implies for such type crystals the type-II components have the potential to replace type-I ones and obtain important NLO applications in the future.

[1]  Xianfeng Chen,et al.  Large acceptance of non-collinear phase-matching second harmonic generation on the surface of an anomalous-like bulk dispersion medium. , 2014, Optics express.

[2]  Guiling Wang,et al.  High-average-power 266 nm generation with a KBe₂BO₃F₂ prism-coupled device. , 2014, Optics express.

[3]  M. Galimberti,et al.  Numerical evaluation of ultrabroadband parametric amplification in YCOB , 2014 .

[4]  E. Shi,et al.  Crystal growth and characterization of 4 in. YCa4O(BO3)(3) crystal , 2014 .

[5]  Yan-qing Lu,et al.  Introduction: Nonlinear Optics (NLO) 2013 feature , 2014 .

[6]  I. Georgescu Symphony of lights , 2012, Nature Physics.

[7]  Zhi‐zhan Xu,et al.  Experimental demonstration of joule-level non-collinear optical parametric chirped-pulse amplification in yttrium calcium oxyborate. , 2012, Optics letters.

[8]  Valentin Petrov,et al.  Diode-pumped mode-locked Yb:YCOB laser generating 35 fs pulses. , 2011, Optics letters.

[9]  Zhengping Wang,et al.  Efficient high-power self-frequency-doubling Nd:GdCOB laser at 545 and 530 nm. , 2011, Optics letters.

[10]  K. Petermann,et al.  Continuous-wave and modelocked Yb:YCOB thin disk laser: first demonstration and future prospects. , 2010, Optics express.

[11]  S. Grechin NONLINEAR OPTICAL PHENOMENA: Integral criterion for selecting nonlinear crystals for frequency conversion , 2009 .

[12]  P. Tidemand-Lichtenberg,et al.  First measurement of the nonlinear coefficient for Gd(1-X)Lu(X)Ca(4)O(BO(3))(3) and Gd(1-X)Sc(X)Ca(4)O(BO(3))(3) crystals. , 2007, Optics express.

[13]  Yiting Fei,et al.  Large-aperture YCOB crystal growth for frequency conversion in the high average power laser system , 2006 .

[14]  D. Armstrong,et al.  Measurement of the chi^(^2^) tensor of GdCa~4O(BO~3)~3 and YCa~4O(BO~3)~3 crystals , 2005 .

[15]  B. Boulanger,et al.  Linear and nonlinear optical properties of the monoclinic Ca 4 YO(BO 3 ) 3 crystal , 2004 .

[16]  M. Richardson,et al.  Non-critical phase-matched second harmonic generation in GdxY1-xCOB , 2003 .

[17]  Gerard Aka,et al.  Crystal growth and optical properties of rare earth calcium oxoborates , 2002 .

[18]  Zhengping Wang,et al.  Non-critical phase matching of GdxY1-xCa4O(BO3)3(GdxY1-xCOB) crystal , 2001 .

[19]  W. Jiyang,et al.  Anisotropy of Nonlinear-Optical Property of RCOB (R= Gd, Y) Crystal , 2001 .

[20]  Y. Mori,et al.  90° Phase-Matching Properties of YCa4O(BO3)3 and GdxY1-xCa4O(BO3)3 , 2001 .

[21]  S. Payne,et al.  Nonlinear optical properties of LaCa(4)O(BO(3))(3). , 2001, Optics letters.

[22]  Z. Shao,et al.  Intracavity second-harmonic generation of 1.06 μm in GdCa4O(BO3)3 crystals , 2001 .

[23]  Jiao Y. Y. Lin,et al.  Determination of the nonlinear optical coefficients of YCa 4 O(BO 3 ) 3 crystal , 2000 .

[24]  Gerard Aka,et al.  Comparative evaluation of GdCOB and YCOB nonlinear optical properties in principal and out of principal plane configurations for the 1064 nm Nd:YAG laser frequency conversion , 2000, LASE.

[25]  K. Petermann,et al.  Type-I non-critically phase-matched second-harmonic generation in Gd1-xYxCa4O(BO3)3 , 1999 .

[26]  T Sasaki,et al.  Noncritically phase-matched frequency conversion in Gd(x)Y(1-x)Ca(4)O(BO(3))(3) crystal. , 1999, Optics letters.

[27]  Shengxia Zhang,et al.  Structural analysis of nonlinearities of Ca4ReO(BO3)3 (Re = La, Nd, Sm, Gd, Er, Y) , 1999 .

[28]  Petra Becker,et al.  Borate Materials in Nonlinear Optics , 1998 .

[29]  François Salin,et al.  Linear- and nonlinear-optical properties of a new gadolinium calcium oxoborate crystal, Ca 4 GdO(BO 3 ) 3 , 1997 .

[30]  Hiroyuki Furuya,et al.  Crystal Growth and Optical Characterization of Rare-Earth (Re) Calcium Oxyborate ReCa4O(BO3)3 (Re=Y or Gd) as New Nonlinear Optical Material , 1997 .

[31]  T. Yamanaka,et al.  Temperature Dependence of Phase-Matching Angle of Second and Third Harmonic Generation in Type-II KDP Crystal , 1986 .